Magnetic propulsion motor

ABSTRACT

The present disclosure relates to a magnetic motor including a drive magnet, a motion magnet, and an acceleration field. The drive magnet includes magnetic shielding, typically on a portion thereof, altering the magnetic field of the drive magnet. In some embodiments, the motion magnet has a cross-section that is generally in the shape of a ‘V’ or ‘A’. The acceleration field is created by the interaction between the drive magnet and the motion magnet as the motion magnet is passed through the altered magnetic field of the drive magnet. The altered magnetic field of the drive magnet may often be near a first end of the drive magnet. In further embodiments, the motion magnet can be operably coupled to an output shaft and rotate around the central axis of the output shaft. The present disclosure, also relates to a device, including the magnetic motor, for generating energy from a turbine.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a continuation-in-part of U.S. patent applicationSer. No. 12/135,614, filed Jun. 9, 2008, published as U.S. patentpublication 2008-0303365, which is a continuation of U.S. patentapplication Ser. No. 11/617,852, filed Dec. 29, 2006, now U.S. Pat. No.7,385,325, which is a continuation of International application numberPCT/US2005/023704, filed Jun. 30, 2005, which claims priority to U.S.provisional patent application Ser. No. 60/584,298, filed Jun. 30, 2004,all of which are hereby incorporated by reference in their entirety.

FIELD OF THE INVENTION

The present disclosure relates to a magnetic propulsion motor and powertransmission system. In particular, the present disclosure relates to amotor and gearing system, wherein power and/or torque is generated usingmagnets and magnetic fields. Magnets are accelerated through themagnetic fields creating a rotational movement about an axis.

BACKGROUND OF THE INVENTION

Magnetic propulsion has traditionally not worked effectively in the pastdue to magnetic lock. That is, it takes as much energy to enter into amagnetic field as is generated leaving the field.

Present magnetic propulsion motors have not been effective indiminishing or eliminating magnetic lock. Present motors use a magneticfield that creates either an attracting force or a repelling force, butnot both. Additionally, present motors do not take into considerationthe shape of the motion magnets or the effect, in certainconfigurations, that magnetic shielding can have. Thus, present motorsare generally inefficient.

Therefore, there is a need in the art for a magnetic propulsion motorthat eliminates or mitigates magnetic lock. The present disclosurerelates to a magnetic propulsion motor without the disadvantagesembodied in present motors.

BRIEF SUMMARY OF THE INVENTION

The present disclosure, in one embodiment, relates to a magnetic motorincluding a drive magnet, a motion magnet, and an acceleration field.The drive magnet includes magnetic shielding, typically on a portionthereof, altering the magnetic field of the drive magnet. In someembodiments, the motion magnet has a cross-section that is generally inthe shape of a ‘V’ or ‘A’. The acceleration field is created by theinteraction between the drive magnet and the motion magnet as the motionmagnet is passed through the altered magnetic field of the drive magnet.The altered magnetic field of the drive magnet may often be near a firstend of the drive magnet. In further embodiments, the motion magnet canbe operably coupled to an output shaft and rotate around the centralaxis of the output shaft. In still further embodiments, a second motionmagnet can be operably coupled to the output shaft at a location that islongitudinally up or down shaft from the first motion magnet. The firstmotion magnet and the second motion magnet may further be radiallyoffset from one another around the output shaft. A second drive magnetcan be added, and another acceleration field may be created by theinteraction between the second drive magnet and the second motion magnetas the second motion magnet is passed through the altered magnetic fieldof the second drive magnet.

The present disclosure, in another embodiment, relates to a method ofcreating a magnetic acceleration field. The method includes altering themagnetic field of a drive magnet, and intermittently passing a motionmagnet proximate the drive magnet to create an interaction between themagnetic fields of the motion magnet and the drive magnet, such that theinteraction causes the motion magnet to be driven away from the drivemagnet. In some embodiments, altering the magnetic field of the drivemagnet includes magnetically shielding a portion of the drive magnet.The method may further involve operably coupling a drive assembly,having an input shaft, to the drive magnet such that the drive magnetrotates around the central axis of the input shaft and is configured tomove the drive magnet away from the motion magnet, and return the drivemagnet proximate to the motion magnet. In some embodiments, a windmillblade can be operably coupled to the input shaft to drive the inputshaft.

The present disclosure, in yet another embodiment, relates to a devicefor generating energy from a turbine. The device includes a turbine, amagnetic motor, a rotatable drive axle, and a rotatable motion axle. Themagnetic motor includes a drive magnet, a motion magnet, and anacceleration field. The drive axle is operably coupled to the drivemagnet and the turbine, wherein rotation of the turbine causes rotationof the drive axle and rotation of the drive axle causes the drive magnetto rotate around a central axis of the drive axle. The motion axle isoperably coupled to the motion magnet and an electrical generator, suchthat rotation around a central axis of the motion axle by the motionmagnet causes the motion axle to rotate and drive the electricalgenerator.

While multiple embodiments are disclosed, still other embodiments of thepresent disclosure will become apparent to those skilled in the art fromthe following detailed description, which shows and describesillustrative embodiments of the present disclosure. As will be realized,the invention is capable of modifications in various obvious aspects,all without departing from the spirit and scope of the presentdisclosure. Accordingly, the drawings and detailed description are to beregarded as illustrative in nature and not restrictive.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a side view of one embodiment of a magnetic propulsion motorof the present disclosure.

FIG. 2 is a schematic view of one embodiment of a multiple chamber,magnetic propulsion motor of the present disclosure.

FIG. 3 is a schematic view of one embodiment of an acceleration fieldgenerator of the present disclosure.

FIG. 4 is a perspective view of one embodiment of a spinner assembly ofthe present disclosure.

FIG. 5A includes several views illustrating one embodiment of a pushmagnet of the present disclosure without magnetic shielding.

FIG. 5B includes several views illustrating one embodiment of a pushmagnet of the present disclosure with one configuration of magneticshielding.

FIG. 6 is a schematic view of the magnetic fields created by oneembodiment of shielded push magnets and shielded motion magnet of thepresent disclosure.

FIG. 7A is a schematic view of one stage of one embodiment of pushmagnets and motion magnets of the present disclosure in operationillustrating a first motion magnet in home position.

FIG. 7B is a schematic view of a second stage of one embodiment of pushmagnets and motion magnets of the present disclosure in operationillustrating a first motion magnet exiting the acceleration fieldgenerator and a second motion magnet entering the acceleration fieldgenerator.

FIG. 7C is a schematic view of a third stage of one embodiment of pushmagnets and motion magnets of the present disclosure in operationillustrating a second motion magnet in home position.

FIG. 7D is a schematic view of a fourth stage of one embodiment of pushmagnets and motion magnets of the present disclosure in operationillustrating a second motion magnet exiting the acceleration fieldgenerator and a third motion magnet entering the acceleration fieldgenerator.

FIG. 8 is a top and side view of one embodiment of a motion magnet ofthe present disclosure.

FIG. 9A is a side view of one embodiment of a rotating hub of thepresent disclosure.

FIG. 9B is a side view of one embodiment of the present disclosure of arotating hub with adjustable arc length between motion magnets.

FIG. 10 is schematic view of one embodiment of a push magnet coupled toan electromagnet of the present disclosure.

FIG. 11 is a side view of one embodiment of a parallel magneticpropulsion motor of the present disclosure with multiple motion hubsaround a single drive hub.

FIG. 12 is a schematic view of one embodiment of a parallel magneticpropulsion motor of the present disclosure with a multiple drive hubsaround a single rotating hub.

FIG. 13A is a schematic view of multiple drive hubs and rotating hubswherein motion and drive magnets are in the same orientation along theirrespective drive and motion axes.

FIG. 13B is a schematic view of multiple drive hubs and rotating hubswherein the motion and drive magnets are in an offset or helicalorientation along their respective drive and motion axes.

FIG. 14 is a schematic view of one embodiment of the present disclosurein which the motion magnets are laterally adjacent to the drive hub.

FIGS. 15A-C include several views illustrating one embodiment of a drivemagnet of the present disclosure, showing the generation of theacceleration field.

FIG. 16 is a view of a wind turbine incorporating one embodiment of theparallel motor of the present disclosure.

DETAILED DESCRIPTION

The present disclosure relates to a magnetic propulsion motor and powertransmission system. More specifically, the present disclosure relatesto a system and method of generating power and/or torque by usingmagnets and magnetic fields. Output of power and/or torque is obtainedfrom rotating motion magnets through one or more magnetic accelerationfields created by drive magnets. The number and arrangement of magnetscan be adjusted to affect output speed, power and/or torque.

According to one embodiment of the present disclosure shown in FIG. 1, amagnetic propulsion motor 100 comprises at least one accelerationchamber 105 (shown in FIG. 2) within main frame 400. Each accelerationchamber 105 includes at least one acceleration field generator 110 andat least one motion magnet 120 and a rotating hub 130 coupled thereto.As described in more detail below and shown in FIG. 9A, the rotating hub130 generally comprises a base 370 and an extension arm 380 for eachmotion magnet 120. The extension arm 380 secures the motion magnet 120to the base 370.

The rotation of the rotating hub 130 causes each motion magnet 120 topass through a magnetic acceleration field created by an accelerationfield generator 110. With reference to FIGS. 1 and 3, an accelerationfield generator 110 comprises two spinner assemblies 135, each spinnerassembly 135 having a spinner axle 140 and two push magnets 150. As seenin FIG. 4, spinner assembly 135 further includes two magnet cradles 170,each magnet cradle 170 rotatably coupling the push magnets 150 tospinner axle 140 such that two push magnets 150 freely rotate, or“spin,” about the spinner axle 140. Referring back to FIG. 1, anacceleration chamber within the main frame 400 further comprises a mainaxle 160 coupled with the rotating hub 130. The rotating hub 130 isrotationally secured to the main axle 160 such that hub 130 and motionmagnets 120 may rotate about the axle 160.

In alternate embodiments, the magnetic propulsion motor 100 may havemultiple acceleration chambers 105, as shown in FIG. 2. In suchsituations, the rotating hub 130 of each chamber 105 may be coupled witha separate axle 160. Alternatively, the rotating hub 130 of any one ofthe chambers 105 may share an axle 160 with any number of hubs 130 ofthe remaining chambers 105. Where multiple hubs 130 share the same axle160, torque and/or power are increased. Therefore, any desired amount ofpower can be achieved by adding more chambers 105.

In one embodiment of the present disclosure, shown, for example, in FIG.1, a magnetic propulsion motor 100 comprises two acceleration fieldgenerators 110. In other embodiments, it may be desirable to have moreor fewer acceleration field generators 110. Typically, the accelerationfield generators 110 are evenly placed circumferentially around therotating hub 130 such that the motion magnets 120 pass through theacceleration field created by each of the acceleration field generators110, as will be described in further detail.

With reference to FIGS. 3 and 4, an acceleration field generator 110generally comprises two spinner assemblies 135. In alternateembodiments, an acceleration field generator 110 may comprise more orfewer spinner assemblies 135. Each spinner assembly 135 has two pushmagnets 150 that are securely attached to a spinner axle 140 by housingeach push magnet 150 in a magnet cradle 170 rotatably attached to thespinner axle 140 and that rotate relative to the spinner axle 140. Inalternate embodiments, each spinner assembly 135 may comprise more orfewer push magnets 150. The push magnets 150 are typically situated onsubstantially opposing sides of the spinner axle 140. The push magnets150 may be neodymium iron boron (neodymium) rare earth magnets. However,those skilled in the art will recognize that other known magnets mayalso be used for the push magnets 150. The kind of magnet used as thepush magnet 150 may have an effect on the strength of the repulsiveand/or attractive forces acting on a motion magnet 120 in anacceleration field, since various kinds of magnetic materials may differin their amount of magnetic strength.

Another factor that may affect the strength of the magnetic forcesgenerated within an acceleration field is the separation distance or gapbetween push magnets 150 and motion magnets 120 as they rotate past eachother in the acceleration field. In general, the strength of attractiveand repulsive forces between two magnets is in an inverse relationshipwith the distance between the magnets, decreasing rapidly as the gapbetween the magnets increases. This property may be used in several waysduring the operation of various embodiments of the present disclosure.

For instance, in order to control or adjust the power and/or torqueoutput in various embodiments of the present disclosure, the rotationalpaths of the motion 120 and push 150 magnets may be moved closer orfarther away from each other. This may be accomplished, for example, bythe positioning of the main 160 and spinner 140 axles, adjustments tothe size and positioning of the rotation hubs 130 and spinner assembly135, and/or the positioning of the motion magnets 120 and push magnets150.

The inverse relationship between the distance between two magnets andthe strength of attractive and repulsive magnetic forces created thereinmay also be a factor in aiding entry and exit from an acceleration fieldin some embodiments of the present disclosure. The rotation of therotation hubs 130 and spinner assemblies 135 causes motion magnets 120and/or push magnets 120 to rotate closer to and farther away from eachother. For example, motion magnet 120 may rotate into and enter anacceleration field when a push magnet 150 has been rotated by a spinnerassembly 135 to be farther away from motion magnet 120, as discussedbelow and shown in FIGS. 7A-D. The repulsive magnetic force between thetwo magnets is decreased, which may allow the motion magnet 120 to enterthe acceleration field. When motion magnet 120 has entered theacceleration field, spinner assembly 135 may rotate push magnet 150closer to the motion magnet 120 to increase the repulsive magneticforces between the magnets, pushing the motion magnet out of theacceleration field.

In various embodiments of the present disclosure, the shape andorientation of the motion and push magnets may also be adjusted toaffect the distance between the two magnets as they rotate past eachother. For example, an angled profile of a motion magnet 120 may causethe distance between the surfaces of the motion magnet and a push magnet150 to vary as the motion magnet rotates past the push magnet.

Although repulsive and/or attractive forces in general diminish withincreasing distance between two magnets, the forces between two magnetsare also significantly affected by the shape of the magnetic field ofthe individual magnets. Magnets usually have non-uniform magneticfields, such that field strength at all points at a given distance froma magnet surface is not constant. Thus, the repulsive and/or attractiveforces between magnets depend not only on their distance from eachother, but on their orientation and position relative to the shape oftheir respective magnetic fields. The dimensions and shape of a magneticfield for an individual magnet may be affected by magnet shape and thepresence of magnetic shielding. Push magnets 150 and motion magnets 120of the present disclosure may be shaped, oriented, and/or shielded tocreate an acceleration field and generate torque and/or power and reduceor eliminate magnetic lock.

Thus, with reference to FIG. 4, in one embodiment of the presentdisclosure, in addition to housing and securing push magnets 150, themagnet cradle 170 may provide magnetic shielding for push magnets 150,wherein the cradle 170 covers all or part of some of the faces of thepush magnet 150 and appropriately redirects the magnetic force emanatingfrom those faces. Because a magnetic field must always start at one poleand end at the other, magnetic shielding does not actually block amagnetic field. However, magnetic shielding may redirect a magneticfield through the shield, similar to a conductor, so that the magneticfield has lessened or no influence on objects passing by the magnet orside of the magnet that has magnetic shielding.

According to one embodiment of the present disclosure, as depicted inFIGS. 4 and 5B, the magnet cradle 170 covers all or part of all faces ofthe push magnet 150 except for the outermost face 180 and one end edge190. Thus, the magnetic forces emanating from the exposed faces 180 and190 are greater than the magnetic forces emanating from the unexposedfaces. A magnetic field 200 created by a push magnet 150 without suchshielding is depicted in FIG. 5A, whereas an example of the magneticfield 200 created in the acceleration field generator 110 with theshielding of magnet cradle 170 is depicted in FIG. 5B. With furtherreference to FIG. 4, end edge 190, which is exposed and not shielded, isconfigured to face each motion magnet 120 as it enters the accelerationfield. A shielded end edge 280 of push magnet 150 opposes end edge 190and is configured to face each motion magnet 120 as it exits theacceleration field. The outermost face 180 of the push magnet 150closest to motion magnet 120 faces inward towards the motion magnet 120as it passes through the acceleration field.

Magnetic shielding material is desirably material with magneticpermeability. That is, material that will allow magnetic flux lineswithin it. Materials with higher magnetic permeability provide bettermagnetic shielding than those materials with lower magneticpermeability. In one embodiment, the magnet cradle 170 is typicallymanufactured from steel. Alternatively, those skilled in the art willrecognize that other materials may be used to create the same effect foraltering the magnetic field 200.

The two push magnets 150 of a spinner assembly 135 are generallypositioned on opposite sides of the spinner axle 140, as illustrated inFIGS. 3 and 4. The outermost face 180 of the push magnet 150 on one sideof the spinner axle 140 generally has the opposite polarity (i.e.,north) than the polarity (i.e., south) of the outermost face 180 of thepush magnet 150 on the opposite side of the same spinner axle 140, as isdescribed in more detail below with reference to the motor 100 inoperation. The spinner assemblies 135 are generally situated such thatthere is a spatial gap 310 between them large enough for a motion magnet120 to pass through, as seen in FIG. 3.

In a further embodiment of the magnetic propulsion motor 100, anacceleration field generator 110 may comprise a plurality of spinneraxle bearings 210 fixedly attached to the main frame 400. Each spinneraxle 140 may pass through at least one spinner axle bearing 210 allowingthe spinner axle 140 to rotate within the axle bearing 140. A spinneraxle bearing 210 may be manufactured from any material known in the art,such as plastic, aluminum, stainless steel, etc. The friction betweenthe spinner axle 140 and the spinner axle bearing 210 is sufficientlylow to facilitate rotation of the push magnet 150.

Each spinner axle 140 may include at least one belt pulley 220 arrangedat an end of the spinner axle 140, as shown in FIGS. 1, 3, and 4. A belt230 may be arranged around the belt pulley 220 of each spinner axle 140.Thus, all spinner axles 140 will rotate in unison.

A power supply 240 may further be provided to drive the rotation of thespinner axles 140. The power supply 240 may be an electric motor or anyother means capable of driving the spinner axles 140. Where a belt 230and belt pulley 220 system is employed, the power supply 240 may be usedto drive the rotation of a first spinner axle 140, while the belt 230and belt pulleys 220 will transfer the power to rotate the remainingspinner axles 140.

As described, an acceleration chamber 105 of the magnetic propulsionmotor 100 of the present disclosure further comprises at least onemotion magnet 120. The motion magnets 120 are typically neodymium rareearth magnets; however, other magnets known in the art may be usedinstead of the neodymium magnets. The motion magnets 120 generally havethe shape of the letter “V”, “U,” or “A” as shown in FIGS. 6 and 7A,when viewed from the proximal end of the extension arm 380. Inoperation, the shape of the motion magnets 120 helps optimize themagnetic force exerted on the motion magnets 120 by the push magnets150, as illustrated in FIG. 6. Generally, a motion magnet 120 with a “V”or “A” or similar shape, has two extensions 330 and 340, as shown inFIG. 7A, and the two extensions have opposite magnetic polarity. Forexample, referring to motion magnet 120A in FIG. 7A, extension 340 has anorth polarity and extension 330 has a south polarity.

Similar to the push magnets 150, the motion magnets 120 may further havemagnetic shielding 175 to appropriately redirect the magnetic forceemanating from desired edges. As shown in FIG. 8, according to oneembodiment of the present disclosure, magnetic shielding 175 may coverall or part of the surfaces located at the end of the extensions of themotion magnet 120. Additionally, magnetic shielding 175 may be securedto the upper 260 and lower 270 edge surfaces. Magnetic shielding 175, inone embodiment, may create a magnetic field around the motion magnet 120that will interact more efficiently with the magnetic acceleration fieldcreated by the push magnets 150. Alternatively, the magnetic shielding175 may aid in reducing or eliminating magnetic lock by limiting therepelling force created by the push magnets 150 acting against themotion magnet 120 as the motion magnet 120 enters the acceleration fieldgenerator 110. The magnetic shielding 175 is typically manufactured fromthe same material as the shielding material used for manufacturing themagnetic cradles 170.

As shown in FIG. 9A, the rotating hub 130 generally comprises a base 370and at least one extension arm 380. The extension arm 380 connects themotion magnet 120 to the base 370. In one embodiment of the presentdisclosure, a chamber 105 of the magnetic propulsion motor 100 hasmultiple motion magnets 120, and each motion magnet 120 is fixedlycoupled to base 370 of rotating hub 130 by using an extension arm 380.Thus, the number of extension arms 380 coincides with the number ofmotion magnets 120. In alternative embodiments, each extension arm 380may have more than one motion magnet 120. Each extension arm 380 isattached at one end to the base 370 such that the extension arms 380 aregenerally equally spaced circumferentially around the base 370. Thisarrangement appropriately balances the hub 130. At the opposite end ofeach extension arm 380, a motion magnet 120 is attached such that whenthe extension arms 380 are rotating in a forward motion, the open end ofthe “V” or “A” shaped motion magnets 120 enters into the spatial gap 310of the acceleration field generator 110 before the vertex of the motionmagnets 120, thereby causing ends 250 to enter the gap 310 first. Thelength of the extension arms 380 may be increased or decreased dependingon the specific application. In a further embodiment, a chamber 105 ofthe magnetic propulsion motor 100 further comprises a main axle 160coupled with the base 370, wherein the axle 160 rotates relative to thebase 370.

According to one embodiment of the present disclosure, a chamber 105 ofthe magnetic propulsion motor 100 is configured to operate as follows.Rotating hub 130 is aligned such that a motion magnet 120 at the distalend of each extension arm 380 will pass through the spatial gap 310 ofeach of the acceleration field generators 110. In one embodiment,multiple extension arms 380 rotate along with rotating hub 130.Typically, it is desirable to provide an even number of extension arms380 and motion magnets 120 to allow for the polarity of each edge 330and 340 of the motion magnets 120 to be alternated, as shown in FIG. 9A.Not to be limited by theory, it is believed that having motion magnetsof alternating polarity allows a motion magnet to have added attractiveforce to help “pull” it forward, the attractive force coming from theacceleration field immediately preceding it. Not to be limited bytheory, the amount of added attractive force from adjacent accelerationfields may also be affected by the distance between alternating motionmagnets of opposite polarity, as discussed below. Alternatively, theremay only be one extension arm 380 and motion magnet 120.

An embodiment of present disclosure in which the rotation hub 130 isconfigured to carry one or more motion magnets 120 at adjustabledistances or radii from the center of rotation hub 130 is shown in FIG.9B. One or more motion magnets are fixedly or removably attached tomotion cradles 122, which may then be adjustably attached to rotationhub 130, at various distances from the center of the hub. The one ormore motion cradles 122 may be removably attached to a rotation hub 130by any suitable means, for example, by one or more fasteners 126attached through holes 127 in the rotation hub. As multiple motionmagnets 120 are attached closer to the center of motion hub 130, thedistance or arc length 125 between adjacent motion magnets 120 typicallydecreases. The distance or arc length 125 between motion magnets 120 maybe adjusted to a distance or length that maximizes the power and/ortorque output. Alternatively, by adjusting the arc length 125, powerand/or torque outputs as measured by any suitable measuring device, maybe adjusted, for example, to give increased power and/or torque,increased output efficiency, or provide a specific or predeterminedpower or torque output suitable for a particular use. Further, it isalso possible to easily add or remove motion magnets 120 to affect powerand/or torque output for a particular use.

Typically, each motion magnet 120 will be placed equidistant from thecenter of the rotating hub 130. However, the motion magnets 120 may beplaced at alternating or distinctive distances from the center of therotating hub 130 in some embodiments.

As previously described, a chamber 105 of the magnetic propulsion motor100 shown in FIG. 1 may comprise two acceleration field generators 110,each with a set of spinner assemblies 135. Alternatively, more or feweracceleration field generators 110 may be desirable for a particularapplication, and the motor shown in FIG. 1 may be modified accordingly.Generally, where more torque or power is desired, additionalacceleration field generators 110 may be added. Furthermore, theacceleration field generators 110 can generally be evenly placed aroundthe circumferential path of the motion magnets 120 and equidistant fromthe center of the rotating hub 130. Where two acceleration fieldgenerators 110 are used, they typically can be placed on opposite sidesof the circumferential path of the motion magnets 120, as shown in FIG.1.

In some embodiments of the present disclosure, spinner assemblies 135and rotating hubs 130 may be configured to have a gearbox functionality,that is, to increase or decrease the gear ratio between a spinner axle140 and main axle 160, which increases or decreases the RPM of an outputmain axle 160 relative to an input spinner axle 140. Since a spinnerassembly 135 and rotating hub 130 in the present disclosure do notphysically interlock as in conventional gearing, use of the spinnerassembly 135 and rotating hub 130 can create, in effect, a nearlyfriction-free, highly efficient gearbox. In addition, lack of physicalinterlocking avoids mechanical wear to the moving parts, minimal heatgeneration, and has little need for lubrication. A further advantage ofthe motor of the present disclosure is that two or more motion magnets120 evenly spaced around the rotating hub 130 may self-correct therotating hub 140 into the proper orientation and speed if the rotationspeeds of the spinner assembly and rotation hubs begin to run out ofphase because of shock loading or unusually rapid changes in velocity ofthe spinner axle 140, for example. Under the same conditions, aconventional gearbox may be expected to lock, jam, or break,necessitating off-line time and repairs.

Various gear ratios, for example but not limited to 1:1, 1:2, 2:1, 1:3,or 1:4, may be created by increasing or decreasing the number of magnetson a spinner assembly 135 and/or rotating hub 130 in an accelerationchamber 105. For example, a spinner assembly 135 with the same number ofpush magnets 150 as motion magnets on a rotating hub 130 in anacceleration chamber 105 will typically have a 1:1 gear ratio, and thespinner assembly and rotating hub may have the same RPM. Increasing thenumber of motion magnets 120 on a rotating hub 130 relative to thenumber of push magnets 150 on a spinner assembly 135 in the sameacceleration chamber 105 typically decreases the gear ratio, decreasingthe RPM of an output main axle 160. For example, an acceleration chamber105 with two push magnets 150 on a spinner assembly 135 and four motionmagnets on a rotating hub 130 would have a gear ratio of 2:1, i.e., therotating hub 140 would have one-half the RPM as the spinner assembly.Conversely, increasing the number of push magnets 150 on a spinnerassembly 135 relative to the number of motion magnets 120 on a rotatinghub 130 typically increases the gear ratio. For example, an accelerationchamber 105 with four push magnets 150 on a spinner assembly 135 and twomotion magnets 120 on a rotating hub 130 would typically have a gearratio of 1:2, where the rotating hub has twice the RPM of the spinnerassembly. Other gear ratios may be produced with other configurations ofmotion magnets and push magnets.

The magnetic motor of the present invention is generally highlyefficient. A minimal loss of efficiency may be caused by air drag on thespinning parts. In some embodiments, air drag may be reduced by anappropriate airfoil or operation of the motor in a vacuum or a reducedpressure atmosphere.

As previously described, in one embodiment of the present disclosure,each acceleration field generator 110 comprises two spinner axles 140,each having two push magnets 150 rotatable thereabout. The outermostfaces 180 of the two push magnets 150 on the same spinner axle 140 haveopposite polarities. Furthermore, the acceleration field generator 110is typically configured such that, at any given moment, the outermostface 180 of the push magnet 150 facing into the gap 310 on one of thespinner assemblies 135 has the opposite polarity of the outermost face180 of the push magnet 150 facing into the gap 310 on the other spinnerassembly 135, as shown in FIGS. 7A and 7C. Push magnets 150 are alignedin such a manner due to the edges 330 and 340 of the motion magnets 120having opposite polarities, as previously discussed.

In embodiments where more than one extension arm 380 is provided,extension arms 380 may be ordered around the hub such that the motionmagnet edges 330 and 340 alternate polarities from one motion magnet 120to the next. For example, as illustrated in FIG. 7B, motion magnet 120Ahas a north polarity on edge 340 and a south polarity on edge 330, whilethe next subsequent motion magnet 120B has a south polarity on edge 340and a north polarity on edge 330. This alternating pattern may befollowed for all remaining motion magnets 120, which results in an evennumber of extension arms 380 and motion magnets 120.

In operation the push magnets 150 and the motion magnets 120 worktogether to create motion, torque, and power. Magnetic lock occurs inother systems when the motion magnets 120 require as much power to enterthe magnetic field created by the acceleration field generator 110 as isgenerated leaving the magnetic field. In various embodiments of thepresent disclosure, the push magnets 150 are taken out of position toaffect the conflicting magnetic field created by the motion magnets 120and then brought back into the proper position at the appropriate time,thereby eliminating or mitigating magnetic lock. When push magnets 120are removed or reintroduced into the proper position too early or toolate, the motor 100 would lose torque and power. The timing of themotion of the push magnets 150 and the motion magnets 120 of the presentdisclosure allows for the creation of an acceleration field, andmagnetic lock can be significantly reduced or bypassed.

According to one aspect of the magnetic propulsion motor 100 of thepresent disclosure, the timing of the positioning of the push magnets150 in relation to the motion magnets 120 that reduces or avoids themagnetic lock is now described. The positioning of the push magnets 150of the present disclosure will be described with reference to a spinningmotion of push magnets 150. However, other motions or combination ofmotions creating a similar effect can be employed, such as moving,vibrating, pushing, pulling, raising and/or lowering the push magnets150 away from the motion magnets 120 at the appropriate time. Theoverall effect of the motion is to bring the push magnets 150 away fromthe magnetic field of the acceleration field generator 110.

Referring to FIGS. 7A, 7B, 7C and 7D, the push magnets 150 have beennumbered 150A, 150B, 150C and 150D for easier reference while describingthe magnetic propulsion motor 100 in operation. Similarly, the motionmagnets 120 that are visible in these drawings have been numbered 120A,120B and 120C. In FIGS. 7A-D, a longitudinal view showing anacceleration chamber from above is depicted at the top of each figure,and at the bottom of each figure is a projection of an end view of eachcorresponding spinner assembly 135, in order to help show theorientation of the push magnets 150A-D within each spinner assembly.

Referring now to FIG. 7A, motion magnet 120A is in a “home” position.Home position represents the position at which a motion magnet 120 isapproximately equidistant from the entrance and exit of the accelerationfield. Typically, this point is where the motion magnet 120 ispositioned generally at the midpoint of distance 390. At home position,the push magnets 150B and 150C, which are nearest the motion magnetedges 330 and 340 and are part of separate spinner assemblies 135, aregenerally facing one another directly.

The two directly facing push magnets 150B and 150C, thus described, haveopposite polarities. For example, as shown in FIG. 7A, push magnet 150Bhas a south polarity while push magnet 150C has a north polarity.Additionally, as illustrated earlier, each push magnet 150B and 150Cwill have the same polarity as the nearest edge of the motion magnet120A, which is at the center of the acceleration field. For example, asshown in FIG. 7A, push magnet 150B and motion magnet edge 330 both havea south polarity while push magnet 150C and motion magnet edge 340 bothhave a north polarity. This creates the repelling force to acceleratethe motion magnet 120A through the acceleration field. The field createdin gap 310 may also create an attracting force to pull in the nextsubsequent motion magnet 120B, as shown in FIG. 7B. In some embodiments,the rotating hub acts as a flywheel, and inertial forces may help tomove, or may be the predominant force moving the next subsequent motionmagnet 120B into the acceleration field. These forces cause rotating hub130, and therefore motion magnets 120, to rotate about main axle 160.

Meanwhile, as belt 230 causes belt pulley 220 to rotate each spinneraxle 140 in unison, push magnets 150A and 150C rotate to an “upward”position and push magnets 150B and 150D rotate to a “downward” position,as seen in FIG. 7B. Additionally, motion magnet 120A exits theacceleration field generator 110 and magnet 120B enters the accelerationfield generator 110. During this motion, the spinner assemblies 135continue to rotate such that the push magnets 150 are equidistant fromthe center of gap 310, as illustrated in FIG. 7B. This is generally thesame position that the spinner assemblies 135 are in as the nextapproaching motion magnet 120B nears the entrance to the accelerationfield generator 110.

Referring now to FIG. 7C, as motion magnet 120B is nearing the entranceto the acceleration field generator 110, push magnets 150A and 150Dcontinue to rotate relative to the spinner axles 140 such that they willbe approaching a position where they will be directly facing oneanother. When motion magnet 120B enters into this second “home” positionas shown in FIG. 7C, push magnets 150A and 150D will generally bedirectly facing one another. As previously illustrated, when motionmagnet 120B is in home position, push magnet 150A and motion magnet edge330 both have the same polarity, i.e., north, while push magnet 150D andmotion magnet edge 340 similarly have the same polarity, i.e., south. Asdescribed earlier, this creates both the repelling force to expel motionmagnet 120B from the acceleration field and attract motion magnet 120Cinto the acceleration field. The inertia of the spinning rotation hub130 may also help to move motion magnet 120C into position. Oneillustration of the magnetic field lines created in one embodiment ofthe present disclosure wherein a motion magnet 120 is in substantiallythe home position is depicted in FIG. 6.

While motion magnet 120B is exiting the acceleration field generator110, the spinner assemblies 135 will generally be rotating such that thepush magnets 150 are equidistant from the center of gap 310, asillustrated in FIG. 7D. This is generally the same position that thespinner assemblies 135 are in as the next approaching motion magnet120C, having similar characteristics as motion magnet 120A, nears theentrance to the acceleration field generator 110. Alternatively, motionmagnet 120C could be motion magnet 120A rotating through theacceleration field generator 110 once again.

The timing of the position of the push magnets 150 and motion magnets120, thus described, provides for at least two resulting effects. First,an exiting motion magnet, e.g., motion magnet 120A, will be pushed awayfrom the acceleration field, while the next subsequent motion magnet,e.g., motion magnet 120B, which is entering the acceleration field, willbe attracted towards the acceleration field. Second, the push/pulleffect, thus described, extends the duration of the torque resultingfrom the rotation of the hub 130. This duration lasts for approximatelythe time during which a motion magnet 120 passes along the length of apush magnet 150. Each motion magnet 120 passing through an accelerationfield generator 110 will feel both an attracting force entering thefield and a repelling force exiting the field. This dual action can, ina sense, double the duration that a motion magnet 120 is being acted onby magnetic forces. Whereas employing solely a push technique or a pulltechnique would result in a shorter, staccato-like duration.Furthermore, as previously mentioned, the push/pull effect reducesmagnetic lock or backlash effect. Backlash happens where the forces ofthe push magnets 150 want to reverse the forward motion of the motionmagnets 120. Backlash is avoided in various embodiments of the presentdisclosure, because a motion magnet 120 that is approaching anacceleration field generator 110 is attracted toward the generator 110and then repelled out.

In general, for various embodiments of the present disclosure, anacceleration field generator 110 may alter the magnetic accelerationfield within the generator 110 to significantly reduce the repulsiveforce acting on the motion magnet as the motion magnet enters theacceleration field and increase the repulsive force acting on the motionmagnet once the motion magnet has entered the acceleration field. Thus,backlash forces may be significantly reduced compared to the push orpropulsive forces acting on the motion magnet, thus generating motion,torque and/or power. As shown above for one embodiment of the presentdisclosure, the alteration of the acceleration field within theacceleration field generator 110 may be accomplished by rotation of thepush/drive magnet in and out of proximity to the motion magnet. Othermovements of the push/drive magnets, such as moving the push/drivemagnets in and out of position on oscillating arms, are within the scopeof the present disclosure.

In another embodiment of the motor of the present disclosure, anelectromagnet 151 may be coupled to or positioned near a stationary pushmagnet 150, as shown in FIG. 10. Instead of moving the push magnet toalter the acceleration field, the acceleration field may be altered byusing an electromagnet to alter the magnetic field of the push magnet.While FIG. 10 depicts a example embodiment where the electromagnet 151is coupled to the proximal end of the push magnet 150 (proximal to theentrance of the acceleration field), other locations for theelectromagnet are possible, for example, but not limited to, anelectromagnet coupled to or positioned near the distal end of the pushmagnet 150 or at any other place near the push magnet 150. Whenelectrical current flows through electromagnet 151, the magnetic fieldof electromagnet 151 may alter the magnetic field of push magnet 150.Typically, the flow of current into electromagnet 151 can be timed suchthat current flows through the electromagnet 151 and alters the magneticfield of push magnet 150 when a motion magnet 120 is approaching theacceleration field. The alteration of the magnetic field of push magnet150 may reduce the repulsion between the push magnet and motion magnet120, allowing the motion magnet to enter the acceleration field.Typically, the current to electromagnet 151 is turned off when motionmagnet 120 has entered the acceleration field, allowing the repulsiveforce of push magnet 150 to reestablish itself and repel motion magnetout of the acceleration field. Similarly, the flow of electrical currentto electromagnet 151 may be turned on and off by any suitable device.

Other methods of regulating the acceleration field using anelectromagnet and a push magnet are possible. For example, electromagnet151 may be normally always ‘on’ during operation of the motor 100, butthe amount of current may be increased or decreased to alter thestrength of the magnetic field of electromagnet 151 and the extent towhich electromagnet 151 alters the magnetic field of push magnet 150.Further, it is recognized that other appropriate times for energizingthe electromagnet may facilitate a motion magnet 120 entering andexiting an acceleration field. Further yet, in some embodiments, theelectromagnet may be turned “on” once the motion magnet has entered anacceleration field to increase the repulsive force causing the motionmagnet to leave the acceleration field.

In another embodiment of the present disclosure, the push magnet may bean electromagnet. The electromagnet may be coupled to a device that mayreduce or shut off the flow of electrical current to an electromagnet asa motion magnet approaches the acceleration field, and turns on orincreases the current significantly reducing or eliminating backlashagainst the motion magnet.

Accordingly, reducing the repulsive force of the drive/push magnets atthe appropriate time, whether by moving the drive magnets out of theacceleration field, applying techniques of electromagnetism, and/orother methods opens a “window” for a motion magnet to enter anacceleration field by reducing the repulsive force acting against it.Similarly, increasing the repulsive force at the appropriate time,either by moving the push magnets into the acceleration field, orcreating or reestablishing a repulsive force by techniques ofelectromagnetism and/or by other methods after the motion magnet hasentered the acceleration field closes the “window,” propelling themotion magnet out of the acceleration field.

Various embodiments of the magnetic propulsion motor 100 create energywithout pollution. The motors 100 of the present disclosure can be usedto replace any constant RPM motor, such as pumps, electric motors,generators or compressors. There are no size limitations or restrictionsinhibiting the use of the magnetic propulsion motor 100 of the presentdisclosure. Furthermore, the motor 100 may be used as a gearbox toincrease or decrease input RPM, and or increase or decrease power and/ortorque, depending on the configuration of the motor 100.

In the above embodiments, the input spinner axles 140 are generally atright angles to the output main axle 160, thus the output force issubstantially at a 90° or perpendicular direction relative to the inputforce. See, e.g., FIG. 1. In some situations, however, it can beadvantageous or desirable for the input drive axle and output axle to bein the same direction, i.e., parallel to each other.

In that respect, FIG. 11 depicts another embodiment of the presentdisclosure, where a magnetic propulsion motor 500 contains at least onemotion magnet 520 coupled to a motion hub 530. A motion hub 530 may berotationally coupled to a motion axle 560. A motion hub 530 may compriseat least one attachment base 670, which projects laterally from themotion axle 560 and may be a point of attachment for one or more motionmagnets 520, thus securing the motion magnets 520 in the properorientation. In this example embodiment, a motion magnet 520 may beattached to the inner surfaces 671 of two attachment bases 670 at one ormore points on the upper and lower edge surfaces of the motion magnet520. Various other methods of securing the motion magnets 520 in theproper orientation are possible, for example, attachment of motionmagnets directly to the motion axle 560, or attachment of motion magnetsto one or more extension arms that are attached to one or moreattachment bases 670 or directly to the motion axle 560.

The rotation of the rotating motion hub causes each motion magnet 520 topass through a magnetic acceleration field 590 created by anacceleration field generator 510. An acceleration field generator 510contains a drive axle 540, and a rotating drive hub 545 rotatablycoupled to the drive axle 540, and at least one drive or “push” magnet550, which may be typically located along and attached to the outercircumference of the drive hub 545. In this example embodiment, thedrive magnets 550 are attached directly to the drive hub 545, butvarious other methods of attachment of the magnets 550 to the drive hub545 are possible, such as securing drive magnets 550 into magnet cradlesattached to a drive hub 545. The drive magnets 550 are thus secured tothe drive hub 545 in an orientation suitable to create one or moreacceleration fields 590. Other methods of securing drive magnets 550 inthe proper orientation are possible, such as securing the drive magnets550 to one or more extension arms, for example.

Output motion axles 560 and input drive axle 540 are generally parallelto each other. Drive hub 545 generally rotates in the same rotationplane as motion hub 530. The motion hub 530 and drive hub 545 may beheld in close proximity through spaced motion axle bearings 575 anddrive axle bearings that hold the motion axle 560 and drive axle 540,respectively, in place while allowing them to each spin freely. Thebearings 575 may be held in a frame 700. The frame can be substantiallysolid as depicted here, or in any configuration that allows drive axle540 and motion axles 560 to rotate freely in position and from oneanother.

The rotation of motion hub 530 causes motion magnet 520 to pass throughan acceleration field 590 created by the interaction of the motionmagnet 520 and drive magnets 550. Each motion hub 530 may have one ormore motion magnets 520 attached thereto, and each drive hub 545 mayhave one or more drive magnets 550 attached thereto. In one embodiment,the motion hub 530 and drive hub 545 may rotate in opposite directions,causing each motion magnet 520 and drive magnet 550 to rotate inopposite directions past each other as they are brought into proximityduring a portion of their respective rotational paths.

In certain embodiments, the parallel magnetic propulsion motor 500 mayhave multiple rotating motion hubs 530 spaced around a single magneticdrive hub 545 in the same rotation plane, as shown in FIG. 11. Multiplemotion hubs 530 may be spaced equidistantly around a drive hub 545 or inany other suitable configuration. Motion hubs 530 may be coupledindividually to separate motion axles 560.

In the example embodiment shown in FIG. 11, four motion hubs 530 arespaced equidistantly about the perimeter of a single drive hub 545. Twomotion magnets 520 are attached to each of the four motion hubs 530.Four drive magnets 550 are attached to the drive hub 545. Thisconfiguration allows for approximately a four-fold increase in overallpower output over a single motion hub/drive hub configuration (with thesame amount of magnets per drive and motion hub, and the same size driveand motion hub) with little loss in efficiency. In the configurationshown, four motion magnets 520 enter acceleration fields 590 created bythe four drive magnets 550 on the drive hub 545 substantiallysimultaneously.

In other embodiments of a magnetic propulsion motor 500, multiple drivehubs 545 may be spaced around a single motion hub 530 in the samerotation plane, as shown in FIG. 12. Multiple drive hubs 545 may bespaced equidistantly around a motion hub 530 or in any other suitableconfiguration. In the example embodiment shown in FIG. 12, four drivehubs 545 are equally spaced around the perimeter of a single motion hub530, but other suitable numbers of drive hubs and/or spacingconfigurations of drive hubs around motion hub 530 are possible. In theembodiment shown, the motion magnets 520 on the motion hub 530 eachrotate through an acceleration field 590 substantially at the same time.Thus, the torque and power output of a single motion axle 560 can besignificantly increased. The multiple drive axles 540 may be eachpowered by individual power sources, or more than one of the multipledrive axles 540 may be powered by a single power source. In such anembodiment, more than one drive axle 540 may be coupled together bybelts or the like so that they may be rotated by a single power source.

It is recognized that various arrangements of one, two or multiplemotion hubs and one, two or multiple magnetic drive hubs in the samerotation plane are possible. For example, with regard to the exampleembodiment of FIG. 11, the number of motion hubs 530 could be more orless than four, and the number of drive hubs 545 could be more or lessthan four.

In another embodiment of the motor of the present disclosure, shown inFIG. 13A, power and/or torque may be increased by adding motion hubsaxially along a motion axle 560, such that multiple motion hubs may bepresent per motion axle, and rotate in generally parallel rotationplanes to one another. In the example embodiment shown in FIG. 13A, fourmotion hubs 530 are located axially along motion axle 560. However, anyappropriate amount of motion axle 560 output power and/or torque can beachieved by placing one, two or multiple motion hubs on the motion axle.Typically, each motion hub 530 on a motion axle 560 rotates in the samerotation plane as one or more drive hubs 545.

Typically, one or more motion magnets 520 may be attached to each motionhub 530. Where more than one motion hub 530 is attached to a motion axle560, the alignment of motion magnets 520 on each attached motion hub 530may be the same or different as the alignment of the motion magnets onone or more of the other motion hubs attached to the same motion axle.In the embodiment shown in FIG. 13A, motion magnets 520 on each motionhub 530 share substantially the same alignment as motion magnets on theother motion hubs of motion axle 560. In the embodiment illustrated inFIG. 13B, however, the alignment of motion magnets 520 on each motionhub 530 is different from the motion magnets on at least one othermotion hub of motion axle 560.

Generally, where motion magnets 520 on two or more motion hubs 530attached to same motion axle 560 share the same alignment, two or moremotion magnets on the shared-alignment motion hubs will enter intoacceleration fields at the same time. In other words, theshared-alignment motion hubs have a “synchronous” alignment. Wherealignments of motion magnets 520 vary between two or more motion hubs530 attached to the same motion axle 560, motion magnets on thevarying-alignment or “offset”-alignment motion hubs can be configured sothey generally do not enter acceleration fields at the same time. Inthis way, the number of motion magnets 520 in acceleration fields andthe timing of entry into acceleration fields on a motion axle 560 at anyone time may be adjusted to affect power and/or torque output, asdescribed more fully below.

As stated above, FIG. 13A illustrates a synchronous alignment embodimentof the present disclosure. Multiple motion hubs 530 may be orientated ona motion axle 560 such that two or more or all of the motion hubs 530rotate a motion magnet 520 into an acceleration field 590 atsubstantially the same time. Typically, drive hubs 545 and drive magnets550 are arranged in a corresponding alignment to the motion hubs 530 andmotion magnets 520, so that the multiple synchronous acceleration fieldsmay be created. In the example synchronous alignment embodiment shown inFIG. 13A, two motion magnets 520 are equally spaced around the perimeterof each motion hub 530, and four drive magnets 550 are equally spacedaround each of four corresponding drive hubs 545, although any suitablenumber of hubs, magnets per hubs, and magnet spacing configurations arepossible.

Power and/or torque output of the motion axle 560 may have one or moreoutput(s) ‘peaks,’ the peak outputs occurring where motion magnets 520on successive motion hubs 530 synchronously exit acceleration fields.Power and/or torque output may be lower in the intervals between thetimes when motion magnets 520 are exiting acceleration fields.

FIG. 13B illustrates an example embodiment of varying, “offset”alignments, which may give a more constant output of torque and/orpower. In offset alignment embodiments, the motion hubs 530 on the samemotion axle 560 may be offset at one or more offset angles from oneanother, such that motion magnets 520 of one motion hub exit anacceleration field at different times than motion magnets 520 of anothermotion hub. This staggers the times at which motion magnets on the samemotion axle 560 exit acceleration fields, imparting a more constanttorque and/or power to the motion axle 560.

In some offset alignment embodiments, the alignment of one or more of aplurality of motion hubs 530 on the same motion axle 560 may beconfigured such that no motion magnets of any of the one or more motionhubs 530 enter acceleration fields in synchrony with each other. Inother offset alignment embodiments, motion magnets 520 on one motion hub530 may enter acceleration fields in synchrony with one or more of themotion magnets 520 on another motion hub 530 on the same motion axle560, but be offset from one or more of the motion magnets 520 on yetanother motion hub 530 on the same motion axle.

The particular offset alignment of motion hubs 530 attached to the samemotion axle may be characterized by the alignment's “offset angles,”that is, the degree of offset between corresponding motion magnets 520on adjacent motion hubs 530. The offset angle between adjacent motionhubs may or may not be the same between all adjacent motion hubs 530 ona motion axle 560. The offset alignment of drive magnets 550 on adjacentdrive hubs 545 on a drive axle 540 may also be characterized by itsoffset angles.

Typically, drive magnets 550 on one or more drive hubs 545 can bearranged in a offset alignment on a drive axle 540 such that efficientand effective acceleration fields may be created with the correspondingmotion magnets 520 on a motion hub 530.

In some embodiments, the offset angle between adjacent drive hubs 545 onthe same drive axle 540 may be the offset angle between thecorresponding motion hubs on the motion axle 560, adjusted by amultiplier or other variable which is dependent on the gear ratiobetween the corresponding motion hubs 530 and drive hubs 545. Forexample, where a gear ratio between a corresponding drive hub and motionhub is denoted as d:m, then a typical multiplier for the offset angle,D°, for adjacent drive hubs on the drive axle may, in one examplemethod, be approximated by D°=M° (d/m), where M° is the offset anglebetween corresponding adjacent motion hubs on the motion axle.Conversely, M°=D° (m/d) can be used to approximate a typical multiplierfor the offset angle, M°, for adjacent motion hubs on the motion axlewith respect to a known offset for corresponding adjacent drive hubs onthe drive axle. For example, in the embodiment shown in FIG. 13B, thegear ratio is 1:2, i.e., four drive magnets 550 are attached to eachdrive hub 545, and two motion magnets 520 attached to each correspondingmotion hub 530. The offset angle between adjacent drive hubs 545 isabout 22.5°, and thus the offset angle between adjacent motion hubs 530is about 45°. In the example embodiment FIG. 13B, all of the offsetangles between adjacent drive hubs are the same, as well as all of theoffset angles between adjacent motion hubs. However, it is recognizedthat, in some embodiments, not all offset angles between hubs on themotion or drive axles will be the same.

In the example offset alignment embodiment illustrated in FIG. 13B, theoffset angle between corresponding motion magnets 520 is about 45° inthis example, but other suitable offset angles are possible. In a“helical” offset orientation, as is shown in FIG. 13B, each successivemotion hub 530 is offset by the same offset angle in the same directionfrom the previous motion hub 530 on the motion axle 560, but othersuitable alignments are possible, including but not limited torandomized offsetting, whereby each successive motion hub 530 may beoffset from the previous motion hub by any offset, irrespective of theoffset between any other two motion hubs along the same motion axle.

Offset alignments can give a more constant torque output than acompletely synchronous alignment embodiment, such as that shown in FIG.13A. Similarly, offset alignments where none of the motion hubs have thesame alignment, may give a more constant torque than offset, “partiallysynchronous alignments,” where some of the motion hubs have the samealignment.

In some embodiments, multiple motion axles 560, with one, two ormultiple motion hubs 530 positioned axially along the motion axles 560,may be added around the perimeter of a drive axle 540, which may havemultiple drive hubs 545 attached thereto. In other embodiments, one ormore drive axles 540, with one, two or multiple drive hubs 545positioned axially along the drive axles 540 may be positioned aroundone or more multiple motion axles 560 with one, two or multiple motionhubs 530 attached thereto.

The system dynamics of example embodiments of the synchronous andhelical orientations of rotating hubs 130 were modeled in theright-angle motor of the present disclosure, described in detail above,to determine the output torque as a function of angular shaft positionsof both input drive axle 140 and output main axle 160 for variousorientations, with a 3:1 gear ratio reduction, wherein six motionmagnets 120 on a rotation hub 130 were paired with two push magnets 150on a spinner assembly 135. Motion magnets 120 had alternating polaritiesaround the perimeter of the rotating hub 130. This characteristicequation is:

$\begin{matrix}{{T\left( {\theta_{i\; n},\theta_{out}} \right)} = {A_{Config}\mspace{11mu} {\sin \left( {{\frac{\pi}{60}\theta_{out}} - \frac{\pi}{2}} \right)}{{\sin \left( {\frac{\pi}{180}\theta_{i\; n}} \right)}.}}} & {{Eq}.\mspace{14mu} 1}\end{matrix}$

This characteristic equation can be used to simulate numerousconfigurations of motors of the present disclosure, observing behaviorsuch as torque fluctuations, maximum torque loading and so forth. Also,the equation may be able to estimate the torque capacity for anyconfiguration without physically building the configuration. Theequation may be able to model the effects of adding additionalacceleration fields, having different gear ratios, the effects of“helical” offset orientations, and the effects of various sizes ofmagnets. This is all achieved by changing the parameter A_(Config) basedon the number of acceleration fields or other physical parameters of thesystem. The frequencies of the sine wave torque output in the model aredependent on the gear ratios. Phase shifts can be altered to simulate ahelical orientation.

Based on physical experiments with a 3:1 gear ratio embodiment of themotor of the present disclosure, it was determined that the effect oftorque ‘peaks’ in synchronous or single rotating hub per main axleembodiments at high torque loads and/or input speeds from the spinnerassembly 135 was sufficiently small and thus negligible. Thus removingthe effect of torque peaks:

ω_(in)=3ω_(out)

θ_(in)=3θ_(out)+φ  Eq. 2 & 3

where φ is the phase shift between input and output axles. Bysubstituting Equation 3 into Equation 1, we find that the torque is thena sinusoidal function of the output angular position and the phaseshift. It can then be seen that varying amounts of torque are availablefor varying the phase shift. By determining at which phase shift thehighest torque is available, the torque capacity may be determined.

Exceeding that torque may result in a phase shift in which the availabletorque is less than the load and the angular velocity of the outputshaft falls resulting in de-synchronization. For systems without ahelix, this critical phase shift is 270° and by using Equation 3, thismay indicate that just before desynchronization, an opposite pole motionmagnet 120 is directly in the acceleration field as the drive magnet 150enters the acceleration zone. As described above, the motion magnet 120here may slightly lead the push magnet 150 into the acceleration fieldthus resulting in a high repulsion force in the direction of motion. Ifthe phase shift were slightly greater, then the opposite-poled motionmagnet 120 would slightly lag the push magnet 150 resulting in a highrepulsive force against motion thus inducing desynchronization.

In order to determine the load capacity for a given configurationquantitatively the work done by and on the rotation hub/output main axle130, 160 for a single rotation may be modeled as:

$\begin{matrix}{U = {\int_{0}^{2\pi}{{T(\theta)}\ {{\theta}.}}}} & {{Eq}.\mspace{14mu} 4}\end{matrix}$

Because the load capacity is being modeled, it may be assumed that thegear ratio is constant and the phase shift is 270° as we modeled above,and thus T(θ) is known. Assuming that the load torque is constant then:

U _(o)=2πT _(capacity).  Eq. 5

Assuming operation at constant angular velocity (i. θ=0), then the loadcapacity is:

$\begin{matrix}{T_{capacity} = {\frac{1}{2\pi}{\int_{0}^{2\pi}{{T\left( {\theta_{out},\varphi_{critical}} \right)}\ {\theta}}}}} & {{Eq}.\mspace{14mu} 6}\end{matrix}$

where T(θ_(out), φ_(critical)) is the aforementioned modifiedcharacteristic equation for any system configuration. This capacity maybe a slight over-estimation, due to not accounting for losses fromfriction and air resistance, but also assumptions of constant flywheelvelocity.

In actual practice, there may be a slight velocity (and thus anacceleration) sinusoidal fluctuation of the high-inertia rotatinghub/main output axle 130, 160. As mentioned previously, reduction oftorque ‘peaks’ or fluctuations can be minimized by helixing. When thesystem is helixed the torque generated (using Eq. 1, 2, & 3) may have aslightly lower average torque in comparison to a non-helixed averagetorque, but also a lower amplitude. Unlike a non-helixed system,throughout the revolution at no point is the generated torque zero. Ifwe consider:

T _(o) =T _(i)(θ_(out))−I{umlaut over (θ)}(θ _(out))  Eq. 7

where T_(i)(θ_(out)) and {umlaut over (θ)}(θ_(out)) are both sinusoidalfunctions dependent on angular position, as the control, non-helixedsystem and:

A·T _(o) =B·T _(i)(θ_(out))−C·I{umlaut over (θ)}(θ _(out))  Eq. 8

as the helixed system where B<1 and C<1 for some cases, then A>1, thusresulting in slightly higher torque output. Therefore, where the helixdesign may be able to reduce the original acceleration fluctuation by afactor of

$\begin{matrix}\frac{T_{o} - {B \cdot {T_{i}}}}{I{\overset{¨}{\theta}}} & {{Eq}.\mspace{14mu} 9}\end{matrix}$

or greater then the torque capacity can thus be raised above itsoriginal level even if B<1. This results in smoother operation (reduced torque “peaks” orfluctuations) and higher torque capacity in the same space and weight.

As shown in FIG. 14, in alternate embodiments of the parallel magneticmotor of the present disclosure, an acceleration chamber 905 may becreated by two parallel drive hubs 945 rotating laterally adjacent toand flanking a parallel motion hub 930, such that the motion hub 930rotates in a rotation plane between and parallel to the rotation planesof the two drive hubs 945. However, an acceleration chamber 905 may alsobe formed with one drive hub 945 flanking a parallel motion hub 930 insome embodiments. This arrangement of the hubs differs from parallelmagnetic motor embodiments described above where the corresponding drivehub 545 and motion hub 530 rotate in the same rotation plane.

Returning to the example embodiment shown in FIG. 14, drive magnets 950Aand 950B may be attached to flanking drive hubs 945. Drive magnets 950Aand 950B may be attached to drive hubs 945 such that they face inwardinto acceleration chamber 905, in order to interact with motion magnets920 attached to motion hub 930, which is located within the accelerationchamber 905. For example, as shown in FIG. 14, the north face of drivemagnet 950A, and the south face of drive magnet 950B both face inwardinto the acceleration chamber 905. More than one drive magnet 950 may beattached to each drive hub 945, with similar orientations and propertiesas described in detail for drive magnets 950A and 950B. Flanking drivehubs 945 may be rotatably coupled to drive axle 940. Flanking drive hubs945 may be rotatably coupled to the same drive axle 940, as shown inFIG. 14, but other configurations are possible, including attachingflanking drive hubs 945 to different drive axles 940. A drive magnet 950may have magnetic shielding over one or more sides of the drive magnet.The positioning of magnetic shielding on the drive magnet 950 may besubstantially identical to the magnetic shielding on push or drivemagnets (e.g., 150, 450) described in detail above.

One or more motion magnets 920 may be attached to motion hub 930, whichis rotatably attached to motion axle 960. In general, the orientation ofmotion magnets 920 on motion hub 930 is substantially similar to theright-angled embodiments described more fully above and shown, forexample, in FIGS. 1 and 4. Motion magnets 920 may be generally “U”, “V,”or “A” shaped. One or more motion magnets 920 may be held in the properorientation by attachment to the outer edge of an attachment base 970.Other methods of securing motion magnets 920 are possible, such asattachment to extension arms attached to the attachment base 970 ordirectly to motion axle 960. A motion magnet 920 may have magneticshielding over one or more sides of the motion magnet. The positioningof magnetic shielding on the drive magnet 920 may be substantiallyidentical to the magnetic shielding of drive magnets (e.g., 120, 420) aswas described in detail above.

One or both arms of motion magnets 920 are oriented in close proximityto the rotational path of inward-facing drive magnets 950 attached todrive hubs 945 in order to form one or more acceleration fields 990. Forexample, as shown in FIG. 14, a motion magnet 920 may have two arms withopposite polarities, north and south. Drive magnet 950A has aninward-facing side with a north polarity that may interact with an armof the motion magnet 920 to form an acceleration field 990, when rotatedinto close proximity to the motion magnet 920 by drive hub 945. Drivemagnet 950B, attached to drive hub 945 on the other side of accelerationchamber 905, may have an inward-facing side with a south polarity, whichmay rotate typically substantially synchronously with drive magnet 950Ainto close proximity to an arm of motion magnet 920 with a southpolarity to form another acceleration field 990.

As was described in detail above, drive axle 940 may be powered by anysuitable means, such as an internal combustion or electric motor, windpower, etc., for example, which rotates one or more drive hubs 945 withinward-facing drive magnets 950 attached thereto. Repelling forceexerted on one or both arms of motion magnet 920 by one or moreacceleration fields 990 created by the interaction of inward-facingdrive magnets 950 with the arms of motion magnet 920 acts to propelmotion magnet 920 out of the acceleration field 990. This repellingforce acting on motion magnet 920 may cause motion hub 930 to rotate ina rotation plane parallel to the rotation plane of drive hub 945.

Embodiments of the parallel magnetic motor may have a gearboxfunctionality, increasing or decreasing the gear ratios between an inputdrive axle 540 and output motion axle 560. This may be accomplished bychanging the number of magnets on a drive hub 545 and/or motion hub 530rotating in the same rotation plane. For instance, reducing the numberof motion magnets 520 on motion hub 530 relative to the amount of drivemagnets 550 on corresponding drive hub 545 may cause an increased RPM ofthe motion hub relative to the drive hub. Increasing the number of drivemagnets 550 on a drive hub 545 relative to the amount of motion magnets520 on corresponding motion hub 530 may also cause an increased RPM ofthe motion hub relative to the drive hub. In the example embodimentshown in FIG. 11, for example, the number of motion magnets 520 permotion hub 530 may cause the motion hubs 530 and motion axles 560 torotate at twice the speed as the drive hub 545 and drive axles 540.However, various configurations of motion magnets and/or drive magnetare possible to achieve suitable reduced or increased gear ratios, aswas described in detail above.

Because the motion hub 530 and drive hub 545 do not make contact witheach other, an advantage of the gearbox of the present disclosure isthat it generates little or no heat from friction, exhibits littlemechanical wear, and requires little or no lubrication and thus mayrequire much less maintenance or replacement costs than conventionalgear assemblies in which the gears interlock.

A parallel magnetic motor 500 embodiment need not have a gearbox effect.For instance, in the example embodiment shown in FIG. 12, each drive hub545 has four drive magnets 550 and motion hub 530 has four motionmagnets 520, such that the drive hubs and motion hub rotate at the sameRPM.

Whether or not an embodiment of the present disclosure has the same orother gear ratio between the output and input axles, an advantage of thepresent disclosure over motors with gears or other similar connections,is that properly spaced magnets (generally, evenly spaced around thedrive hub 545 and motion hubs 530) can self-correct into the properorientation and speed if the rotation speeds of the drive and motionhubs get out of phase. Under the same conditions, conventional gears orsimilar connections with interlocking parts may be expected to lock, jamor break, necessitating off-line time and repairs.

Drive magnets 550 in parallel motor embodiments may use the same shapes,magnet types and same types and orientation of magnetic shielding forthe drive magnets 150 as detailed for right-angle motor embodiments.That is, magnetic shielding may cover all or part of all faces of thedrive magnet 550 except for the outermost face (facing the motion magnet520) and one end. Those skilled in the art will recognize that otherknown magnet materials, magnet shapes, magnetic shielding, and placementof magnetic shielding may be used for the drive magnets 550.

Motion magnets 520 can be generally the same shape in the parallel motorembodiments as described for motion magnets 120 for the right-angledembodiments of the present disclosure. Thus, motion magnets 520 may begenerally “V,” “U,” or “A” shaped. Similar to the drive magnets 550, themotion magnets 520 may further have magnetic shielding 675 toappropriately redirect the magnetic force emanating from desired edges,which may be substantially similar to the shielding used in on themotion magnets 150 in the right-angled embodiments detailed above. Thatis, magnetic shielding may cover all or part of the surfaces located atthe end of the extensions of the motion magnet 520. Additionally,magnetic shielding may be secured to the upper and lower edge surfaces(see, e.g., FIG. 8). However, those skilled in the art will recognizethat other known magnet materials, magnet shapes, magnetic shielding,and placement of magnetic shielding may be used for the motion magnets520.

A power supply may further be provided to drive the rotation of one ormore drive axles 540. The power supply may be an electric or gasolinemotor or any other means capable of driving the drive axles 540, such aswater power, steam power, or wind power, as shown in FIG. 16 anddescribed in further detail below.

Typically, each motion magnet 520 will be placed an equal distance fromthe center of the motion hub 530. However, the motion magnets 520 may beplaced at alternating or distinctive distances from the center of themotion hub 550 in some embodiments. Similarly, each drive magnet 550 maybe placed an equal, alternating or distinctive distance from the centerof the drive hub 545 in some embodiments.

The positioning of the drive magnets 550 of the parallel embodiments ofthe motor of the present disclosure will be described with reference toa rotating motion of drive magnets 550. However, other motions orcombination of motions creating a similar effect can be employed, suchas moving, vibrating, pushing, pulling, raising and/or lowering drivemagnets 550 away from motion magnets 520 at the appropriate time. Theoverall effect of the motion is to bring the drive magnets 550 away froman acceleration field generator to allow motion magnets 520 to enter theacceleration field generator.

Alternatively, as described more fully above for right-angleembodiments, the required motion of the drive magnets 550 in and out ofproximity to an acceleration field to avoid magnetic lock in parallelembodiments of the present disclosure may be replaced by static,electromagnetic drive magnets, or electromagnetic drive magnets placedin proximity to conventional magnets, in which a magnetic field polaritymay be rapidly altered at appropriate times in order to facilitate theentry and exit of motion magnets into an acceleration field.

The operation of the parallel motor embodiments will now be discussedwith reference to FIGS. 15A, 15B, and 15C. The drive magnets 550 in theparallel embodiments have been numbered 550A, 550B, 550C and 550D foreasier reference while describing the magnetic propulsion motor 500 inoperation. Similarly, the motion magnets 520 that are visible in thesedrawings have been numbered 520A, and 520B.

Referring now to FIG. 15A, motion magnet 520A is at a “home” position,generally with side 630 at the midpoint of side 650 of drive magnet550A, in the center of acceleration field 590. In this embodiment thepolarity of side 630 of motion magnets 520A and 520B is north and side640 is south. Side 650 of drive magnet 550A has a north polarity, i.e.,the same polarity as side 630 of motion magnet 520A. Motion hub 530 anddrive hub 545 rotate in opposite directions. In this example embodiment,drive hub 545 rotates clockwise, as shown by arrow 701 and motion hub530 rotates counterclockwise, shown by arrow 702. The rotation anddirection of rotation of drive hub 454 is driven by a power source, suchas, but not limited to an electric or internal combustion motor, or byalternate means, such as water power, wind power, steam power, etc.

Motion magnets 520A-B and drive magnets 550A-D may have facing sides 630and 650 all with the same polarity, i.e., all-north or all-southpolarities. In some embodiments, the polarities of facing sides 630 and650 may alternate, as described with regard to the right-angleembodiments. However, whenever sides 630 and 650 will directly face eachother in an acceleration field, they should have the same polarity. Thiscreates the repelling force to accelerate motion magnet 520A through andout of the acceleration field 590. This force causes motion magnets520A-B and therefore rotating hub 530 to rotate about main axle 560.

The drive force rotating drive hub 545 clockwise causes drive magnet550A to rotate away from the acceleration field 590 and 550B to rotatetoward it, as shown in FIG. 15B. As can be seen from FIG. 15B, motionmagnet 520A has rotated counterclockwise out of the acceleration field590. At the same time, 520B begins to enter the area where theacceleration field 590 will be created. In this orientation, theacceleration field “window” is open, and the repulsion force betweenmotion magnet 520B and drive magnets 550A and 550B is significantlylower. An acceleration field is once again created as motion magnet 520Bis able to rotate into proximity to drive magnet 550B, which exert arepulsive force against each other.

Thus, motion magnet 520B can more easily enter the acceleration field asshown in FIG. 15C. At this position, drive magnet 550B edge 650, hasrotated into close proximity to motion magnet 520B, edge 630, i.e.,“home” position. As noted above, edge 650 and edge 630 have the samepolarity. As the motion hub 530 and drive hub 545 continue to rotate inopposite directions between the orientations in FIGS. 15B and 15C,motion magnet 520B edge 630 is exposed to the full strength of thecreated acceleration field, between motion magnet 520B and drive magnet550B.

As can be seen, the rotation directions of the motion hub 530 and drivehub 545 lengthens the time that the motion magnet 520B edge 630 spendsin close proximity to the drive magnet 550B edge 650, generatingsignificant repulsive force. Further, the repulsive force caused by theproximity of the same polarity on the drive magnet 550B edge 650 andmotion magnet 520B edge 630 also causes the motion hub 530 to rotatefurther in a counterclockwise direction, imparting torque and/or powerto motion axle 560.

The timing of the position of drive magnets 550 and motion magnets 520,thus described, provides for at least two resulting effects. First, anexiting motion magnet, e.g., motion magnet 520A, will be pushed awayfrom the acceleration field created by an interaction with drive magnet550A, while the next subsequent motion magnet, e.g., motion magnet 520B,which is entering the acceleration field area, faces a much lowerrepulsive force as it enters the acceleration field because drivemagnets 550A and 550B are away from the acceleration filed area asmotion magnet 520B enters. Backlash is avoided in the present disclosurebecause the repulsive force of acting on a motion magnet 520 that isapproaching an acceleration field generator 510 is significantly reducedin this manner.

The magnetic motor of the present disclosure may be used in manydifferent situations, such as electricity generation, pumps, electricmotors, generators or compressors. Further, the motor of the presentdisclosure can be used as a power transmission in a gas-powered orelectric automobile, and in other situations where a low-friction,low-emission motor may be desirable.

An example use of the motor of the current disclosure is within a windturbine, as shown in FIG. 16. In a wind turbine 800, drive axle 540 maybe driven by turbine blades 810 spinning in winds of various velocities.The drive axle 540 extends into a nacelle 820, inside of which there maybe located one or more drive hubs 545 attached to drive axle 540. One ormore push or drive magnets 550 may be attached to each drive hub 545.

As shown in FIG. 16, one or more motion magnets 520 may be attached tomotion hub 530, which may be attached to a motion axle 560. A drive hub545 may be rotated by the action of wind on turbine blades 810, which isimparted to drive hub 545 by drive axle 540, which is operably coupledto turbine blades 810. As described above, drive hub 545 may rotate adrive magnet 550 into proximity to a motion magnet 520 attached tomotion hub 530, which can freely rotate in the same rotation plane asdrive hub 545. An acceleration field may be created by the interactionof drive magnet 550 with motion magnet 520. Acceleration imparted onmotion magnet 520 by the acceleration field may cause motion hub 530 andmotion axle 560 to rotate. Motion axle 560 may be attached to and impartspin on a rotor of generator 830, which may be used to generateelectricity.

As shown in FIG. 16, multiple motion hubs 530 may be present withinnacelle 820. In the example embodiment shown in FIG. 16, only one motionhub 530 is attached per motion axle 560, however, as was described fullyabove, more than one motion hub 530 may be present per motion axle 560.Similarly, any suitable number of motion axles 560 may be utilized. Twodrive hubs 545 are attached to drive axle 540 in the example embodimentin FIG. 16, and are rotated by the action of wind on turbine blades 810.However, one, two, or more drive hubs 545 may be attached to drive axle540 in other embodiments. In the example embodiment of FIG. 16, twomotion hubs 530 are paired with a single drive hub 545, however, as wasdescribed fully above, one, two, or more motion hubs 530 may be rotatedby a drive hub 545.

As was described in detail above, the alignment of multiple motion hubs530 on a motion axle 560 may be synchronous or offset. In offsetalignments, the entry of motion magnets 520 into acceleration fields canbe staggered such that the torque imparted on motion axles 560 by therepelling force acting on the motion magnets 520 can be configured to bemore constant.

An advantage of an embodiment of the wind turbine motor of the presentdisclosure is that by varying the sizes of motion hubs relative to thedrive hub, suitable RPM for electrical generation may be generated inmotion axles 560 by the gearbox properties of the present disclosure.Wind turbines may typically spin a drive axle at a RPM too slow forefficient energy generation; thus, the gear ratio adjustments possiblewith the ability to adjust the size and number of motion magnets 520 permotion hub 530, and/or drive magnet 550 per drive hub 545 may achievesufficient motion axle 560 rotation speeds for electrical generationwithout additional conventional, interlocking gearing.

Furthermore, without interlocking gears, friction can be significantlyreduced, allowing for the use of such turbines at lower wind speeds thanconventional wind turbines. Also, without interlocking parts, high windsor wind bursts that may cause gearboxes of conventional wind turbines tolock up or break may merely cause the motion and drive hubs of thepresent disclosure to slip out of phase. The embodiments of the presentdisclosure allow the out-of-phase hubs to quickly realign on their own.Thus, the embodiment shown in FIG. 16 allows for more efficientgeneration of electricity from wind turbines because of the reduction offriction and the capture of electricity from lower and higher wind speedareas than with turbines with conventional gearboxes. In addition, theremay be reduced maintenance costs because of less frequent breakdownsthan with conventional motors, which have more interlocking parts andmay need more complicated mechanisms to prevent damage to internal gearscaused by excessive wind speeds.

In other embodiments of the motor of the present disclosure, since nomechanical contact is made between the drive magnets and the motionmagnets, the system is allowed to operate through solid, non-magnetic,non-conductive structures without any effect on performance. Forinstance, some components of the motor can be positioned on oppositesides of a wall to transfer energy to, for example but not limited to,clean rooms or bulkheads, etc.

Although the present disclosure has been described with reference topreferred embodiments, persons skilled in the art will recognize thatchanges may be made in form and detail without departing from the spiritand scope of the disclosure. For example, the distance that thepush/drive magnets are from the motion magnets will determine thestrength of the attracting and repelling forces. Similarly, the sizeand/or dimensions of the push magnets and motion magnets will increaseor decrease the strength of the attracting and repelling forces.Changing the strength of the attracting and repelling forces will changethe amount of torque and/or power created. Further, changing the numberof push/drive magnets per spinner assembly or drive hub, and/or motionmagnets per rotating hub or motion hub, will change the torque and powercreated. Further, the number of spinner assemblies per each rotatinghub, drive hubs per motion hub, rotating hubs per each spinner assembly,or motion hubs per drive hubs can also affect the power and/or torquecreated. Changing the number of spinner assemblies powered by eachspinner axle or rotating hubs on each main axle, or drive hubs poweredby each drive axle, and motion hubs per motion axle can also affect thepower and/or torque created. In embodiments where multiple rotating hubsare present on one main axle, offsetting the orientation of the motionmagnets in each rotating hub from the other rotating hubs on the sameaxle, or motion magnets in each motion hub from the other motion hubs onthe same axle can also affect the power and/or torque created.

1. A magnetic motor comprising: a first drive magnet having magneticshielding on a portion thereof altering the magnetic field of the firstdrive magnet; a first motion magnet; and a first acceleration fieldcreated by the interaction between the first drive magnet and the firstmotion magnet as the first motion magnet is passed through the alteredmagnetic field of the first drive magnet.
 2. The magnetic motor of claim1, wherein the altered magnetic field is near a first end of the firstdrive magnet.
 3. The magnetic motor of claim 1, wherein the first motionmagnet has a cross-section that is generally in the shape of a ‘V’ or‘A’.
 4. The magnetic motor of claim 3, further comprising a rotatableoutput shaft wherein the first motion magnet is operably coupled to theoutput shaft and rotates around a central axis of the output shaft. 5.The magnetic motor of claim 4, further comprising a second motion magnetoperably coupled to the output shaft.
 6. The magnetic motor of claim 5,wherein the second motion magnet is operably coupled to the output shaftat a location that is longitudinally up or down shaft from the firstmotion magnet.
 7. The magnetic motor of claim 6, wherein the first andsecond motion magnet are radially offset from one another around theoutput shaft.
 8. The magnetic motor of claim 7, further comprising: asecond drive magnet having magnetic shielding on a portion thereofaltering the magnetic field of the second drive magnet; and a secondacceleration field created by the interaction between the second drivemagnet and the second motion magnet as the second motion magnet ispassed through the altered magnetic field of the second drive magnet. 9.The magnetic motor of claim 1, further comprising a second drive magnethaving magnetic shielding on a portion thereof altering the magneticfield of the second drive magnet, wherein the acceleration field iscreated by the interaction between the drive magnet, the second drivemagnet, and the motion magnet as the motion magnet is passed through thealtered magnetic fields of the drive magnet and the second drive magnetsubstantially simultaneously.
 10. The magnetic motor of claim 4, furthercomprising a rotatable input shaft wherein the first drive magnet isoperably coupled to the input shaft and rotates around a central axis ofthe input shaft.
 11. The magnetic motor of claim 10, wherein the firstdrive magnet rotates around the input shaft in generally the same planeas the first motion magnet rotates around the output shaft.
 12. Themagnetic motor of claim 10, wherein the first drive magnet rotatesaround the input shaft in a plane that is substantially perpendicular tothe plane in which the first motion magnet rotates around the outputshaft.
 13. A method of creating a magnetic acceleration field, themethod comprising: altering the magnetic field of a first drive magnet;and intermittently passing a first motion magnet proximate the firstdrive magnet to create an interaction between the magnetic fields of thefirst motion magnet and the first drive magnet, such that theinteraction causes the first motion magnet to be driven away from thefirst drive magnet.
 14. The method of claim 13, wherein altering themagnetic field of the first drive magnet comprises magneticallyshielding a portion of the first drive magnet.
 15. The method of claim13, wherein altering the magnetic field of the first drive magnetcomprises using an electromagnet proximate the first drive magnet andintermittently energizing the electromagnet to affect the magnetic fieldof the first drive magnet.
 16. The method of claim 13, furthercomprising operably coupling a drive assembly, comprising an inputshaft, to the first drive magnet such that the first drive magnetrotates around a central axis of the input shaft and is configured tomove the first drive magnet away from the first motion magnet, andreturn the first drive magnet proximate to the first motion magnet. 17.The method of claim 16, wherein the drive assembly further comprises awindmill blade operably coupled to the input shaft.
 18. The method ofclaim 16, further comprising operably coupling the first motion magnetto an output axle, such that the first motion magnet rotates around acentral axis of the output axle.
 19. A device for generating energy froma turbine, comprising: a turbine; and a magnetic motor comprising: afirst drive magnet having magnetic shielding on a portion thereofaltering the magnetic field of the first drive magnet; a first motionmagnet; and a first acceleration field created by the interactionbetween the first drive magnet and the first motion magnet as the firstmotion magnet is passed through the altered magnetic field of the firstdrive magnet; a rotatable drive axle operably coupled to the first drivemagnet and the turbine, wherein rotation of the turbine causes rotationof the drive axle and rotation of the drive axle causes the first drivemagnet to rotate around a central axis of the drive axle; and arotatable motion axle operably coupled to the first motion magnet and anelectrical generator, such that rotation around a central axis of themotion axle by the first motion magnet causes the motion axle to rotateand drive the electrical generator.
 20. The device for generating energyof claim 19, wherein the turbine is a wind turbine.